odel damped oscilliations using second order differential equations
odel damped oscilliations using second order differential equations
Fundamental Concepts
- Damped oscillations refer to oscillatory motion where the amplitude decreases over time.
- Damped oscillations are represented mathematically using second order differential equations.
- The general form of a damped oscillation is given by m * y’’ + b * y’ + k * y = 0, where y’‘ represents the second derivative of displacement, y’ represents the first derivative of displacement, m is the mass, b denotes the damping constant, and k denotes the stiffness.
Classification of Damping
- Oscillations can be over-damped, critically damped or under-damped, depending on the value of the damping ratio.
- The damping ratio is calculated by zeta = b / (2 * sqrt(m*k)).
- If zeta < 1, the system is said to be under-damped. The system oscillates, but the amplitude of oscillation decreases over time.
- If zeta = 1, the system is said to be critically damped. This represents the boundary between oscillatory and non-oscillatory systems.
- If zeta > 1, the system is said to be over-damped. In this case, the system does not oscillate.
Calculating Essential Values
- The natural frequency of undamped oscillation can be calculated using w_n = sqrt(k/m).
- The damped frequency can be calculated using w_d = w_n * sqrt(1 - zeta^2). This applies only for under-damped systems.
- The time constant of the system can be given by t = m/b, indicating the time it takes for the displacement to reduce to a certain fraction of its original value.
Solution of The Differential Equations
- The nature of the differential equation’s solution is determined by the type of damping.
- In the case of under-damped systems, the solution is a sum of an exponential decay and an oscillating function, given by y(t) = Aexp(-zetaw_nt)cos(w_d*t + phi).
- In the case of critically damped systems, the solution includes an exponential decay then linear growth, given by y(t) = (A + Bt)exp(-zetaw_nt).
- For over-damped systems, the solution is a sum of two exponential decays, given by y(t) = A* exp(r_1t) + B exp(r_2*t), where r1 and r2 are the roots of the characteristic equation.
End of revision for Damped Oscillations - remember to test your understanding by working through a variety of mathematical problems to consolidate these topics.